2014
DOI: 10.5194/acp-14-2315-2014
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Influence of surface morphology on the immersion mode ice nucleation efficiency of hematite particles

Abstract: Abstract. In this paper, the effect of the morphological modification of aerosol particles with respect to heterogeneous ice nucleation is comprehensively investigated for laboratory-generated hematite particles as a model substrate for atmospheric dust particles. The surface-area-scaled ice nucleation efficiencies of monodisperse cubic hematite particles and milled hematite particles were measured with a series of expansion cooling experiments using the Aerosol Interaction and Dynamics in the Atmosphere (AIDA… Show more

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Cited by 79 publications
(166 citation statements)
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“…First, it could introduce new, physical active sites. For example it has been shown for hematite particles that mechanical milling can change the ice nucleation surface site density, even when accounting for changes in surface area (Hiranuma et al, 2014). Second, it could liberate and/or expose mineral surfaces that were previously encased in volcanic glass.…”
Section: Immersion Freezing Of Droplets Containing Na / Ca Feldsparmentioning
confidence: 99%
“…First, it could introduce new, physical active sites. For example it has been shown for hematite particles that mechanical milling can change the ice nucleation surface site density, even when accounting for changes in surface area (Hiranuma et al, 2014). Second, it could liberate and/or expose mineral surfaces that were previously encased in volcanic glass.…”
Section: Immersion Freezing Of Droplets Containing Na / Ca Feldsparmentioning
confidence: 99%
“…In particular, the dynamic light scattering (DLS) size of suspended illite NX particles (0.05 to 1 mg bulk illite NX sample in 1 mL of double-distilled water) was determined using the StabiSizer ® (Microtrac Europe GmbH, PMX 200CS) over the range of 0.0008 to 6.5 µm hydrodynamic diameter. A more detailed description of this instrument and its application for studying the size of particles in suspension are addressed in Hiranuma et al (2014b), and only a brief discussion is given here. The DLS measurements were carried out with negligible contribution of multiple scattering due to the utilized 180 • backscattering mode.…”
Section: Particle Size Distributionmentioning
confidence: 99%
“…Subsequently, a scanning mobility particle sizer (SMPS, TSI Inc., Model 3081 differential mobility analyzer, DMA, and Model 3010 condensation particle counter, CPC) and an aerodynamic particle sizer (APS, TSI Inc., Model 3321) were used to measure particle size distributions over the range of 0.01 to 15.4 µm volume equivalent diameter. The assumption of particle sphericity, a dynamic shape factor (DSF or χ in equations) of 1.49 ± 0.12 (average of 10 measurements ± standard deviation) and a particle density of 2.65 g cm −3 were used to obtain the geometricbased (volume equivalent) diameter from an APS (Hiranuma et al, 2014b). At MRI-DCECC, a combination of an SMPS (TSI Inc., Model 3936) and a welas ® optical particle counter (welas-OPC, PALAS, Sensor series 2500) was used to acquire a size distribution for the size range of 0.01 to 47.2 µm volume equivalent diameter directly from the 1.4 m 3 volume vessel.…”
Section: Particle Size Distributionmentioning
confidence: 99%
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“…Insensitivity of shape factor toward ice nucleation implies that T1 particles were sufficiently irregular that further increase in irregularity (e.g., T2 particles) does not seem to affect ice nucleating efficiency of ash particles. Experiments with controlled irregular features [e.g., Hiranuma et al, 2014] on the particles would be useful to understand more about the significance of shape factor toward ice nucleation.…”
Section: 1002/2015gl063270mentioning
confidence: 99%